dc.contributor.author |
ANANTH, SUDARSHAN |
en_US |
dc.date.accessioned |
2019-12-24T12:30:57Z |
|
dc.date.available |
2019-12-24T12:30:57Z |
|
dc.date.issued |
2009-08 |
en_US |
dc.identifier.citation |
Fortschritte der Physik Progress of Physics, 57(9), 857-861. |
en_US |
dc.identifier.issn |
0015-8208 |
en_US |
dc.identifier.issn |
1521-3978 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4301 |
|
dc.identifier.uri |
https://doi.org/10.1002/prop.200900062 |
en_US |
dc.description.abstract |
The pure gravity Lagrangian can be written as the “square” of the pure Yang‐Mills Lagrangian to second order in coupling constants. This paper uses this form of the gravity Lagrangian as a starting point to arrive at a compact light‐cone superspace Lagrangian for 𝒩 = 8 supergravity to order κ2. |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Wiley |
en_US |
dc.subject |
Gravity square |
en_US |
dc.subject |
Yang?Mills |
en_US |
dc.subject |
8 Supergravity |
en_US |
dc.subject |
Compact light?cone superspace |
en_US |
dc.subject |
2009 |
en_US |
dc.title |
Gravity as the square of Yang‐Mills: implications for 𝒩 = 8 supergravity |
en_US |
dc.type |
Article |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.identifier.sourcetitle |
Fortschritte der Physik Progress of Physics |
en_US |
dc.publication.originofpublisher |
Foreign |
en_US |